text:
Christopher Bollen Might Be the World's Most Driven Fiction Writer
A day in New York with the novelist, brought to you by Cadillac.
By GQ Bespoke - Sponsor Content
"My agent gave me the best advice," Christopher Bollen confides over coffee at Cafe Luxembourg on the Upper West Side, "which is to always start the next book before a new one comes out. If it's a huge success, it's daunting to try to live up to that success, and if it's a big failure, you don't want to write again. So I always have the next one in mind and get started on it almost immediately."
An art and culture critic, editor-at-large at Interview Magazine, and a four-time novelist, Bollen defies the stereotype of the procrastinating, egocentric writer. He is a passionate devourer of books, a sit-all-day-and-write type, someone who finds researching and editing infinitely more pleasurable than releasing a finished work. "I got really nervous about accepting too many congratulations because I think it stops you," he explains. And so, while Bollen's stylish and suspenseful book, A Beautiful Crime, just hit shelves in January of this year, he's already buried in research for the next one.
One of the secrets to Bollen's success, which keeps him producing so steadily, is his willingness to push into new territory. "Each time I write a book, I take on something that seems phenomenally difficult for me to write about, or a topic I don't really know much about," he explains, "It keeps me entertained and engaged as I'm writing. I could never be the kind of writer who writes about the same two-block radius for his entire career. I'm too curious about what's over the next horizon". Bollen's stories have been set in Venice, Greece, and New York, for example, and his colorful characters have been experts in snakes, sailing, and the silver industry.
Bollen also credits the energy of New York for helping him stay hungry. "I bought this house in The Berkshires a few years ago, a 1920 hunting cabin, thinking it would be the perfect place to write, but I've found that, actually, the best place to write is in my apartment in New York. All of the noise and distraction of New York slips into the book and makes it richer and more stimulating." Instead, Bollen uses his country home to "get curious about nature", read, do research, and contemplate. And the process begins the moment he leaves his home on the Upper West Side and begins the drive up North.
When Bollen bought his place in The Berkshires, he also got a car for the first time in years. "It was like a homecoming to be able to drive again. I didn't realize how much I missed it. And it's actually so good for writing. I can plan out chapters and figure out entire plots while driving through the country. There's something deeply inspiring about being behind the wheel and thinking through a novel in progress. There's a really wonderful union between the road and the page. It's creative." Bollen also relishes the opportunity to listen to the radio, everything from local news to pop stations, to gather inspiration.
Bollen's love of cars and road trips goes back as far as his interest in literature and writing. While the Cincinnati native was devouring mystery novels as a kid, he was also taking in the world through the backseat windows of his mom's Cadillac. "My grandfather was a vintage car collector and he must've told my mom well before I was born that she should only drive Cadillac. About every four or five years she'd get a new one, and she was the only one in the family that could drive it. Her Cadillac was sacred to her." While the car's steady, luxurious ride fueled many childhood daydreams, it also reflected the professional success of his mother, a college professor, and the reward that comes with hard work. Now an accomplished professional himself, Bollen gets to experience those same rewards. The job, the house, the ride.
As for Bollen's ambitions for the future, they are unsurprisingly ever expanding, ever evolving. "When I first became a writer I thought that I would love to write seven books. But now that I've written four, I'm bringing the ideal total up to at least nine," Bollen says with a laugh, concluding, "You know, I think you change the goalpost a little bit as you move along."
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text:
Fermi kinetics transport program models high-speed semiconductor devices better, says study
by University of Illinois Grainger College of Engineering
The commercial hydrodynamics package (left) predicts that electron temperatures can drop below the ambient temperature (300 kelvins, or 80 degrees Fahrenheit in this simulation) while the Fermi kinetics solver (right) gives more reasonable temperature predictions. Credit: The Grainger College of Engineering at the University of Illinois Urbana-Champaign
Electronic devices made from the semiconductor gallium nitride stand to revolutionize wireless communications. They can operate at higher speeds and temperatures than devices made from silicon, so they can be used to control the higher frequency radio waves needed for faster and higher bandwidth data transfer. In addition, their ability to withstand much lower temperatures makes them promising for use in quantum computing. To realize the material's full potential, though, accurate modeling and simulation tools are needed to guide scientists and engineers designing new devices.
The research group of Shaloo Rakheja, a professor of electrical and computer engineering at the University of Illinois Urbana-Champaign, collaborated with Air Force Research Laboratory engineers Nicholas Miller and Matt Grupen to study two semiconductor simulation tools: a commercial hydrodynamics software package, and the Fermi kinetics transport solver developed by Grupen.
Their article, named an editor's pick in the Journal of Applied Physics, reports that the Fermi kinetics solver has mathematical properties that allow it to better handle the extreme conditions under which gallium nitride devices will operate.
"This is the first time a direct comparison has been made between the state-of-the-art commercial program and a custom-developed research code," Rakheja said. "It is important for the semiconductor community to understand the strengths and limitations of each."
According to Rakheja and Miller, the most important difference between the two programs is how they model the electronic heat flow. The commercial package uses Fourier's law, an empirical model that does not necessarily work well for semiconductors, while the Fermi kinetics transport solver uses more fundamental thermodynamic principles for this purpose. The researchers believe that this accounts for the different predictions each program makes.
"There is a strong connection between the underlying physics and the behavior of each program," Rakheja said, "and we wanted to explore that in the context of a device technology that's highly relevant today: gallium nitride."
To compare the two codes, the researchers simulated an elementary gallium nitride transistor with each. They found that the two programs gave similar results under modest operating conditions. However, when they introduced large, transient signals of the kind expected in high-speed applications, they obtained unexpected results for electron temperature from the commercial package. It predicted that at short time scales the electron temperature would dip below the ambient temperature, while the Fermi kinetics solver gave more consistent temperature profiles.
In addition, when they examined the rate of convergence, a mathematical indicator of simulation self-consistency, of each, the Fermi kinetics solver converged faster. The researchers concluded from this that the Fermi kinetics solver is more computationally robust.
Rakheja's group is now using the solver's robustness to simulate more gallium nitride devices. They aim to understand how the material heats up as it operates at high speeds and use this information to design devices that fully take advantage of the material's properties.
"Gallium nitride has really been a game changer," Miller said. "As the technology continues to evolve into more sophisticated forms, a critical component of the development cycle is modeling and simulation of the transistors."
More information: Ashwin Tunga et al, A comparison of a commercial hydrodynamics TCAD solver and Fermi kinetics transport convergence for GaN HEMTs, Journal of Applied Physics (2022). DOI: 10.1063/5.0118104
Journal information: Journal of Applied Physics
Provided by University of Illinois Grainger College of Engineering
Citation: Fermi kinetics transport program models high-speed semiconductor devices better, says study (2022, December 19) retrieved 31 January 2023 from https://techxplore.com/news/2022-12-fermi-kinetics-high-speed-semiconductor-devices.html
New heat model may help electronic devices last longer
Semiconductors with an aligned interface
UV light may illuminate improvements for next generation electronic devices
New method produces robust transistors
Previously theoretical material, a nitride perovskite, synthesized and measured
Gallium nitride processor—next-generation technology for space exploration
Under pressure: Breakthrough new material solves problem of wearable sensors
Scalable method to manufacture thin film transistors achieves ultra-clean interface
Highly performing lithium sulfur batteries based on metallic molybdenum disulfide nanosheets
A system to enable multi-kilometer and sub-terahertz communications at extremely high frequency bands

redpajama_set_name: RedPajamaCommonCrawl


text:
Q: MySQL: AVG function: Why does query return incorrect value? So I ran this small query and I seem to have something strange going on.
I want to display all items that have a stock greater than the average stock in stock (if that makes sense...).
When I run it one of the products has less stock than the calculated average...and I'm not sure why. In this scenario the item returning that should not be is: 421
Return Data:
"sum(quantity_stocked)" "count(product_id)" "avg(quantity_stocked)"
"15885"                 "18"                "882.5000"

"product_id"    "quantity_stocked"
"861"           "1082"
"591"           "1948"
"485"           "1402"
"421"           "858"
"277"           "1920"
"214"           "902"
"59"            "1021"

Queries:
select sum(quantity_stocked), count(product_id), avg(quantity_stocked)
FROM products;

SELECT product_id, quantity_stocked
FROM products
WHERE quantity_stocked > (
    SELECT avg(quantity_stocked)
    FROM products
    GROUP BY product_id
    LIMIT 1
    );

Remaining Code:
CREATE TABLE products
(
product_ID              int(10)             UNIQUE,
product_name            varchar(30)         NOT NULL,
quantity_stocked        int(5),
product_cost            dec(8,2)            NOT NULL,
PRIMARY KEY (product_ID)
);

INSERT INTO products VALUES
(452,'Nike SS Pro Top',418, 22.99),
(861,'Nike LunarGlide 7',1082, 74.99),
(453,'Nike LS Pro Top',654, 64.99),
(454,'Nike SS Pro Top',720, 64.99),
(451,'Nike Pro Tank',480, 45.99),
(485,'Nike 5k Run Short',1402, 24.99),
(582,'Nike Fit Capri',750, 29.99),
(591,'Nike Be Fast Tight',1948, 39.99),
(847,'Nike Legend Tee',120, 34.99),
(277,'Nike Miller v-neck',1920, 44.99),
(135,'Adidas Soccer Pant',630, 34.99),
(456,'Adidas SS Breathe Top',754, 19.99),
(457,'Adidas Pro Cleat',626, 44.99),
(214,'Adidas Slide',902, 19.99),
(054,'Underarmor SL Top',854,54.99),
(059,'Undersarmor LS High Neck',1021,54.99),
(574,'Underarmor TR Short',746,24.99),
(421,'Underarmor TR Balance Shoe',858,84.99);

A: In your subquery, you compare to average of one of your products (which is, in this particular example, will be #452, with quantity_stocked of 418), not average of all products. Just remove this part:
GROUP BY product_id
LIMIT 1

redpajama_set_name: RedPajamaStackExchange


Today is September 1st. In some parts of the world it is officially first day of fall. In many countries in Europe school starts on the 1st. Even Harry Potter boarded Hogwarts Express on the 1st of September.
With fall come many wonderful things - cooler weather, trees dressed up in gold and red, warm sweaters and cups of hot coffee or tea. Fall is cozy and warm and here at Becozi that's what we are all about.
Which is why we are incredibly excited to announce the arrival of our new Merino wool colors. Many of them are simply perfect for fall - take a look at the beautiful plum and mocha, olive and navy and we're convinced you will fall in love with them like we have.
We'd like to officially introduce you to the new colors and show them off so you can pick the one that speaks most to you.
That's right - peach is back! We stocked peach back in 2015 and 2016 but took it out of the running for the last while. But it's back by popular demand - it's perfect for those not willing to let go of light, summery things quite yet and make a blanket that makes you think of slow summer mornings.
Are you as much of a fan of purple tones as we are? We simply can't resist the gorgeous plum. With tones of both purple and a bit of red, it is the perfect warm tone to spice up a neutral bedroom or living room.
Stock up on your plum here.
This beautiful light green, almost a seafoam tone, is perfect for pastel decors as it is delicate and soft. With equal parts of green and blue mixed into it, light green can easily complement both blue-toned as well as green-toned rooms in your house.
Find the light green Merino here.
This dark green is so deep and rich that it reminds us of a stormy sea at twilight, churning with the waves. It makes us think of The Little Mermaid and all things aquatic, as its predominantly blue blend makes it a perfect color for sea enthusiasts.
Buy your dark green here.
Ah, that deep dark green! It reminds us of forest nymphs, morning dew on grass and the color of oak leaves at the end of summer. This would be a beautiful addition to any warm-toned room as the olive will balance it out beautifully.
Grab olive toned Merino here.
This navy is on the gray scale, so a bit more muted in vibrancy. But it complements yellow tones beautifully.
Navy is perfect for both light and dark decors: it can serve as a centerpiece of a light room, a visual heavyweight the eye is drawn to. But it can equally blend beautifully into a darker-toned room with colors such as gray and black.
Buy your navy Merino here.
We can't help it - we love mocha. It makes us think of morning coffee, caramel and toffee - all things we absolutely love. It is an absolute perfect match for light and neutral decors as it warms the room up and makes it more inviting.
Make sure to buy your mocha Merino yarn for fall here.
Don't forget that we are discounting some Merino colors so this is the perfect opportunity to grab some beautiful Merino at an amazing discount. Check out our clearance section here for more products.
So whether it is mocha or plum, make sure to stock up on these beautiful colors today and get started on your next chunky knitting project! Or let us make you the next chunky knit creation that you're going to love.
Love the new colors. Great job.


text:
Ahnentafel, Generation No. 1
Person Not Viewable . He/She was the son/daughter of Person Not Viewable and Person Not Viewable .
Alva Virgil Robinson was born 10 Jul 1923 in Near Federalsburg, Caroline County, Maryland, and died 14 Feb 2002 in Phoenixville, PA. He was buried 20 Feb 2002. He was the son of Frederick "Fred" Charles Robinson and Harriet Moore.
Person Not Viewable . He/She was the son/daughter of Vernon Otto Wright and Lois Annie Shufelt.
Children of Person Not Viewable and Alva Virgil /Robinson/ are:
Person Not Viewable . He/She married Person Not Viewable .
Frederick "Fred" Charles Robinson was born 23 Jul 1881 in Maryland, and died 3 Feb 1949. He was the son of William Henry Robinson and Celia Virginia "Jennie" Wilson.
Harriet Moore was born 22 Nov 1892 in Delaware, and died 9 Jan 1950.
Children of Harriet /Moore/ and Frederick "Fred" Charles /Robinson/ are:
James Charles Robinson was born 6 Mar 1917 in Federalsburg, Caroline County, Maryland, and died 2 Oct 1991 in Easton, Talbot County, Maryland. He married Maude H. Lare on 1975. She was born 29 Nov 1911 in Maryland, and died 30 Dec 1985.
Alva Virgil Robinson was born 10 Jul 1923 in Near Federalsburg, Caroline County, Maryland, and died 14 Feb 2002 in Phoenixville, PA. He married Person Not Viewable .
Person Not Viewable .
Vernon Otto Wright was born 28 Nov 1894 in Choptank, Caroline County, Maryland, and died 2 Dec 2000 in Denton, Caroline County, Maryland. He was buried 5 Dec 2000. He was the son of Charles Jefferson Wright and Annie Emily Harding.
Lois Annie Shufelt was born Aug 1894 in Maryland, and died 11 May 1985. She was the daughter of Elmer Friss Shufelt and Lura E. McMahan.
Children of Lois Annie /Shufelt/ and Vernon Otto /Wright/ are:
Louise Downes Wright was born 21 Dec 1916 in Near Harmony, Caroline County, Maryland, and died 15 Feb 2009 in Denton, Caroline County, Maryland. She married Francis Pierce Adams on 6 Dec 1940. He was born 3 Feb 1919 in Near Concord, Caroline County, Maryland, and died 27 Aug 1998 in Denton, Caroline County, Maryland. He was buried 30 Aug 1998 in Concord Meth Cem, Concord, Caroline County, Maryland.
Person Not Viewable . He/She married Alva Virgil Robinson on 23 Dec 1948. He was born 10 Jul 1923 in Near Federalsburg, Caroline County, Maryland, and died 14 Feb 2002 in Phoenixville, PA. He was buried 20 Feb 2002.
William Henry Robinson was born 16 Jul 1855 in Delaware, and died 5 Nov 1929. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland. He was the son of William Robinson and Eliza Ann Hurat?.
Celia Virginia "Jennie" Wilson was born 20 Nov 1854, and died 30 Jul 1942. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland. She was the daughter of John Wilson and Sarah Ann Todd.
Children of Celia Virginia "Jennie" /Wilson/ and William Henry /Robinson/ are:
Frederick "Fred" Charles Robinson was born 23 Jul 1881 in Maryland, and died 3 Feb 1949. He married Vena "Venie" B. Williamson on Abt 1904. She was born Feb 1882 in Maryland, and died Aft 1910.
Francis Elmer Robinson was born 17 Jul 1883, and died 1 Mar 1940. He married Nellie Edmondson Liden on Nov 1905. She was born 27 Oct 1885, and died 29 Nov 1969.
Cora Virginia Robinson was born 11 May 1885, and died 16 Jan 1965. She married Frederick Palmer Parker on 20 Sep 1905. He was born 19 Feb 1887, and died 18 Jan 1946. He was buried in Hollywood Cem, Harrington, Kent County, Delaware.
William John Robinson was born 15 Dec 1889, and died 7 Feb 1944. He married Mary C. Ross on 10 May 1915. She was born 22 Feb 1891 in Sussex County, Delaware, and died 12 Dec 1953 in Dover, Kent County, Delaware. She was buried 16 Dec 1953 in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Horace Edwin Robinson was born 16 May 1894, and died 20 Jul 1940. He married Anna Pearl Ross on 29 Dec 1920 in Caroline County, Maryland. She was born 19 Apr 1897 in Near Federalsburg, Caroline County, Maryland, and died 17 Sep 1991 in Cambridge, Dorchester County, Maryland. She was buried 21 Sep 1991 in Bloomery Cemetery, Smithville, Caroline County, Maryland.
Charles Jefferson Wright was born 8 Apr 1868. He was the son of Constantine Wright and Mary Ellen Eaton.
Annie Emily Harding was born 7 Apr 1871. She was the daughter of Edmondson Arey Harding and Harriett Catherine .
Children of Annie Emily /Harding/ and Charles Jefferson /Wright/ are:
Vernon Otto Wright was born 28 Nov 1894 in Choptank, Caroline County, Maryland, and died 2 Dec 2000 in Denton, Caroline County, Maryland. He married Lois Annie Shufelt. She was born Aug 1894 in Maryland, and died 11 May 1985.
Elmer Friss Shufelt was born 3 Mar 1869 in Columbia County, New York, and died 20 Aug 1944 in Federalsburg, Caroline County, Maryland. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland. He was the son of Jacob Shufelt and Julia Ann .
Lura E. McMahan was born May 1873 in Maryland, and died 1945. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland. She was the daughter of William Frank McMahan and Eliza Ann "Annie" Andrew.
Children of Lura E. /McMahan/ and Elmer Friss /Shufelt/ are:
Lois Annie Shufelt was born Aug 1894 in Maryland, and died 11 May 1985. She married Vernon Otto Wright. He was born 28 Nov 1894 in Choptank, Caroline County, Maryland, and died 2 Dec 2000 in Denton, Caroline County, Maryland. He was buried 5 Dec 2000.
George Franklin Shufelt was born 3 Jan 1896 in Friendship, Caroline County, Maryland, and died 4 Dec 1987 in Seaford, Sussex County, Delaware. He married Ruth Beatrice Turner on 31 Dec 1919. She was born 16 Feb 1901 in Federalsburg, Caroline County, Maryland, and died 15 Mar 1988 in Seaford, Sussex County, Delaware. She was buried 18 Mar 1988 in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Hattie E. Shufelt was born 9 Feb 1897 in near Friendship, Caroline County, Maryland, and died 10 Mar 1987 in Denton, Caroline County, Maryland. She married Mayo Stewart Woodward. He was born 16 Apr 1894, and died 15 Nov 1931. He was buried in Unity Washington Cemetery, Hurlock, Dorchester County, Maryland.
Lula H. Shufelt was born 20 Aug 1898 in Caroline County, Maryland, and died 25 Jan 1989 in Easton, Talbot County, Maryland. She married Charles Herbert Fearins. He was born 26 Feb 1897 in Harmony, Caroline County, Maryland, and died 5 Dec 1951. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Carl Elmer Shufelt was born 27 Jan 1901 in Maryland, and died 17 Mar 1983 in Easton, Talbot County, Maryland. He married H. Irene Pitts on Abt 1923. She was born 20 Apr 1899 in Maryland, and died Dec 1974.
Jesse Lee Shufelt was born 4 Dec 1904 in Maryland, and died 13 Jul 1977. He married Anna Mae Jump. She was born 6 Nov 1915 in Williamsburg, Dorchester County, Maryland, and died 2 Sep 1989 in Georgetown, Sussex County, Delaware. She was buried 6 Sep 1989 in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Roy Jacob Shufelt was born 3 Mar 1908 in Maryland, and died 3 Feb 1980. He married Person Not Viewable .
Vinton Downes Shufelt was born 21 Mar 1909 in Maryland, and died 8 Aug 1979 in Salisbury, Wicomico County, Maryland. He married Person Not Viewable .
Ernest Friss Shufelt was born 3 Mar 1912 in Maryland, and died 9 Apr 1985. He married Catherine Webster. She was born 19 Mar 1914, and died May 1979.
William Robinson was born Abt 1820 in Delaware, and died 17 Jun 1889 in Near Andersontown, Caroline County, Maryland. He was buried in Bloomery Cemetery, Smithville, Caroline County, Maryland.
Eliza Ann Hurat? was born 21 Feb 1820 in Delaware, and died 29 Jul 1880. She was buried in Bloomery Cemetery, Smithville, Caroline County, Maryland.
Children of Eliza Ann /Hurat?/ and William /Robinson/ are:
Rebecca Robinson was born Abt 1844 in Delaware, and died Bef 25 Nov 1896. She married Joseph Waldis. He was born Abt 1847 in Switzerland, and died Bef 25 Nov 1896.
Martha A. Robinson was born Abt 1845 in Delaware. She married Person Not Viewable .
James Robinson was born Abt 1849-1850 in Delaware, and died Aft 1880. He married Mary Etta Beauchamp. She was born 20 Mar 1854 in Maryland, and died 23 Dec 1890. She was buried in Bloomery Cemetery, Smithville, Caroline County, Maryland.
William Henry Robinson was born 16 Jul 1855 in Delaware, and died 5 Nov 1929. He married Celia Virginia "Jennie" Wilson on 31 Dec 1879. She was born 20 Nov 1854, and died 30 Jul 1942. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Sarah "Sallie" E. Robinson was born 1856 in Delaware, and died 9 Apr 1899. She married William Richard Wright on 28 Dec 1875. He was born 25 Jun 1852, and died 25 Dec 1925.
Margaret "Maggie" E. Robinson was born 29 Jul 1859 in Maryland, and died 14 Nov 1912. She married Cannon Charles Wright on 13 Dec 1877. He was born 7 Nov 1854, and died 23 May 1925. He was buried in Bloomery Cemetery, Smithville, Caroline County, Maryland.
John Wilson was born Abt 1824-1826 in Maryland, and died 13 Jul 1879 in Near Concord, Caroline County, Maryland. He was buried in Bloomery Cemetery, Smithville, Caroline County, Maryland.
Sarah Ann Todd was born 13 Dec 1831 in Maryland, and died Bef 25 Apr 1859.
Children of Sarah Ann /Todd/ and John /Wilson/ are:
William Thomas Wilson was born 8 Aug 1851 in Maryland, and died 6 Jul 1916. He married Martha Cahall on 27 Apr 1877 in Denton, Caroline County, Maryland. She was born 2 Jun 1856 in Delaware, and died 29 Apr 1930. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Henry Francis Wilson was born 16 Aug 1852 in Maryland, and died 2 Feb 1923. He married Elanora Dixon on 29 Apr 1875. She was born 24 Apr 1855 in Maryland, and died 22 May 1910. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Celia Virginia "Jennie" Wilson was born 20 Nov 1854, and died 30 Jul 1942. She married William Henry Robinson on 31 Dec 1879. He was born 16 Jul 1855 in Delaware, and died 5 Nov 1929. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Charles Edward Wilsondied Bef 1860.
Constantine Wright was born 19 May 1834 in Maryland, and died 26 Jun 1869.
Mary Ellen Eaton was born Abt 1844 in Maryland, and died 28 Aug 1876.
Children of Mary Ellen /Eaton/ and Constantine /Wright/ are:
Lewis Richard Wright was born 17 Jun 1859 in Maryland, and died 19 Oct 1944. He married Sarah Martha Gootee on Abt 1885. She was born 27 Feb 1862 in Maryland, and died 1909. She was buried in Belmont Cem, Choptank, Caroline County, Maryland.
Edward Everett Wright was born 4 Jun 1861 in Maryland, and died 25 Mar 1888. He married Lucetta Phillips on 17 Nov 1883. She was born 16 Jun 1860 in Maryland.
Annie Eliza Wright was born 12 Jun 1864. She married James Warner Oldfield on 26 Mar 1885. He was born 14 Jun 1856.
Sarah Jane Wright was born 13 Apr 1866. She married John Henry Dennis on 17 Jan 1894. He was born 4 Sep 1870.
Charles Jefferson Wright was born 8 Apr 1868. He married Annie Emily Harding on 6 Jan 1892. She was born 7 Apr 1871.
Edmondson Arey Harding .
Harriett Catherine .
Children of Harriett Catherine // and Edmondson Arey /Harding/ are:
Annie Emily Harding was born 7 Apr 1871. She married Charles Jefferson Wright on 6 Jan 1892. He was born 8 Apr 1868.
Jacob Shufelt was born 25 Oct 1821 in New York, and died 24 Mar 1893. He was buried in Springhill Cemetery, Easton, Talbot County, Maryland.
Julia Ann was born 17 May 1824 in Columbia County, New York, and died 9 Mar 1900 in near Friendship, Caroline County, Maryland. She was buried in Springhill Cemetery, Easton, Talbot County, Maryland.
Children of Julia Ann // and Jacob /Shufelt/ are:
Emma C. Shufelt was born 1 Mar 1850 in New York, and died 25 Oct 1926.
Anna W. Shufelt was born 18 Mar 1854 in New York, and died 18 Jun 1903. She married Chauncey D. Garvey. He was born Nov 1845 in New York, and died Aft 10 Jul 1920. He was buried in Union Grove Cem, Harmony, Caroline County, Maryland.
Mary E. Shufelt was born 2 Sep 1859 in Hudson, New York, and died 12 Nov 1933 in Near Federalsburg, Caroline County, Maryland. She married James Spry Willis on 16 Feb 1878 in Near Easton, Talbot County, Maryland. He was born 6 Feb 1840 in Caroline County, Maryland, and died 7 Jun 1925. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Elmer Friss Shufelt was born 3 Mar 1869 in Columbia County, New York, and died 20 Aug 1944 in Federalsburg, Caroline County, Maryland. He married Lura E. McMahan on 28 Jan 1891 in Caroline County, Maryland. She was born May 1873 in Maryland, and died 1945. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
William Frank McMahan was born Feb 1850 in Maryland, and died 1935. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Eliza Ann "Annie" Andrew was born Aug 1852 in Maryland, and died 1925. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Children of Eliza Ann "Annie" /Andrew/ and William Frank /McMahan/ are:
Lura E. McMahan was born May 1873 in Maryland, and died 1945. She married Elmer Friss Shufelt on 28 Jan 1891 in Caroline County, Maryland. He was born 3 Mar 1869 in Columbia County, New York, and died 20 Aug 1944 in Federalsburg, Caroline County, Maryland. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Thomas Linwood McMahan was born 14 Apr 1876 in Caroline County, Maryland, and died Nov 1952. He married Mary J. Majors on 4 Jan 1899 in Hynson, Caroline County, Maryland. She was born Dec 1881 in Maryland, and died Aft 1920.
Elizabeth "Bessie" A. McMahon was born 1877 in Maryland, and died 9 Sep 1969. She married Thomas Wilbur Hampton Collins on 20 Mar 1907 in Hurlock, Dorchester County, Maryland. He was born 7 Dec 1878 in East New Market, Dorchester County, Maryland, and died 4 Jan 1953 in East New Market, Dorchester County, Maryland. He was buried in East New Market Cem, East New Market, Dorchester Co., Maryland.
Altha Elsie McMahan was born 26 Apr 1880 in Maryland, and died Aft Feb 1963. She married William John Sard on 19 Sep 1900 in Hurlock, Dorchester County, Maryland. He was born 23 Feb 1878 in Maryland, and died 18 May 1951. He was buried in East New Market Cem, East New Market, Dorchester Co., Maryland.
C. Nelson McMahon was born 9 Nov 1881 in Caroline County, Maryland, and died 6 Mar 1953 in Near Federalsburg, Caroline County, Maryland. He married Corinne B. Collins. She was born 28 Jun 1888 in Maryland, and died 18 Jul 1968.
William Vinton McMahon was born Sep 1884, and died 1919. He married Margaret Helen Satterfield on 1 Apr 1912 in Concord, Caroline County, Maryland. She was born Aug 1888 in Maryland, and died 1962. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Arthur Sherman McMahon was born 31 Dec 1886, and died Jul 1972. He married Lelia Jane Smith. She was born Jan 1888 in Maryland, and died 1972. She was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Emma H. McMahan was born 17 Dec 1888 in Maryland, and died 9 Nov 1970. She married Dennis R. Nichols on Jul 1916 in Caroline County, Maryland. He was born 3 Feb 1877 in Maryland, and died 7 Dec 1944. He was buried in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Herman A. McMahan was born 20 Dec 1890 in Maryland, and died 15 Feb 1963 in Baltimore, Maryland. He married Minnie E. Smith. She was born 9 Oct 1892 in Maryland, and died 30 Apr 1914 in Hagerstown, Washington County, Maryland. She was buried 3 May 1914 in Hillcrest Cem, Federalsburg, Caroline County, Maryland.
Frank Earle McMahan was born Jan 1893, and died Aft Feb 1963.


text:
We're proud to announce that Macquarie Capital, an active participant in the Australian real estate sector, has become a PIF National Donor. It's a great fit between our organisations.
Macquarie Capital Executive Director and Head of Real Estate ANZ, Antony Green, said Macquarie Group, through the Macquarie Group Foundation, focuses on supporting social and economic opportunities for young people in the communities where we live and operate.
"We know that homelessness or unstable housing poses significant barriers to accessing opportunity for young people and Macquarie supports a number of community organisations working in the area of youth disadvantage, including addressing homelessness," he said.
"We recognise that youth homelessness is a significant issue and we welcome the opportunity to be part of the solution by providing our support to PIF."
Macquarie Capital is looking forward to collaborating with PIF to make a real impact on the issue.
The donor relationship is a continuation of Macquarie's long-standing support and commitment to PIF. Murray Coleman OAM, Head of Development Projects, Macquarie Capital, is on the PIF National Board of Directors and Macquarie was an early sponsor of the PIF Regatta on Sydney Harbour.
Stay up-to-date on everything happening at PIF. Subscribe to our enews.


The Great War naturally brought many changes to the world, but those changes were also felt here locally in the Waco area. The construction of two military bases inside the city proper, Camp MacArthur and Rich Field, had a huge impact on the city's size, demographics, and economy. Local schools and universities suddenly had to contend with a new wartime dynamic in their daily operations, and many German Americans found themselves in tenuous situations as a wave of patriotic fervor swept the nation. In addition, a terrible flu epidemic took its toll on local soldiers and citizens alike.
The Baylor University Institute for Oral History (BUIOH) is proud to present a series of interview excerpts from the archives of BUIOH chronicling the WWI era in Waco. Highlights from nine interview series are available containing the perspectives of individuals ranging from an established political family to rural German American immigrants. This content represents approximately half of the discovered materials covering local topics on WWI. Further interviews are currently being processed for digitization and will be added as they become available.
Interviews in this section are featured on a new software platform recently installed on the Baylor campus named the Oral History Metadata Syncronizer, or OHMS for short. OHMS allows the user to simultaneously engage audio/video with a transcript or index. The WWI in Waco project is the first from BUIOH to employ this technology. The interviews listed below have complete topical indexes to browse - simply click on a topic and select "Play Segment" to advance to that point in the narrative.
Pre-War Topics: Cotton Palace, parades, downtown theaters, circuses and promotions, Waco as "The Athens of Texas"


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Laverne Cox Is ***FLAWLESS on the Cover of TIME
It finally happened.
Remember when Laverne Cox didn't make TIME's 100 Most Influential People in the World list and people were rightfully mad? (She'd placed fifth in the online poll.) This is better news: Cox is now the magazine's cover girl. (The cover is not a response to the backlash, though, a TIME spokesperson told Buzzfeed; it has been in the works for months.)
The issue, which features a story about the growing transgender rights movement, is on stands June 9; a Q&A with Cox is online now. Choice excerpt:
"I was in sixth grade and I was going through puberty. During puberty, the attraction for other boys got really strong. And I learned in church that was a sin. I imagined that my grandmother was looking down on me and that she knew what I was thinking, because she's in heaven. I just imagined that I was disappointing her and it just was devastating for me. So I went to the medicine cabinet and got a bottle of pills. And took them. And swallowed them. And went to sleep, hoping not to wake up. And I did wake up, with a really bad stomachache. I don't remember what the pills were. Whatever it was, I thought that they would kill me but they didn't."
Now on a lighter note: Orange Is the New Black returns June 6.
Laverne Cox Is Producing a Documentary About Transgender Teens for MTV
Photo Credit: Time
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South Africa was ranked amongst the countries with the poorest performance in Mathematics and Science, the City has identified and acknowledged this poor results and has rolled out a mechanism to eradicate this predicament. The Municipality believes in taking ownership of the challenges that are faced by the country and as a result, takes action in finding solutions for the future.
The Office of the Deputy City Manager: Support Services is mandated to implement the Science, Technology, Engineering and Mathematics (STEM) Programmes seeing as the City has identified the rapid increase in scarce skills within the Province and in South Africa at Large.


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This Is Horrifying! Watch Gov Whitmer Brainwash Children About Lockdowns
Michigan Governor Gretchen Whitmer (Democrat) recently had a discussion with Santa Claus that turned into total insanity. Kids were given a lecture about how the elves at the North Pole are actually wearing their masks!
Fancy that. The kids were given yet another message about the importance of following the rules and staying safe.
Of course, the children wanted to know if Santa Claus was still wearing his mask. They were also concerned about whether the virus was running rampant at the North Pole. Santa Claus proceeded to tell the kids about the masks at his workshop and he claimed that all his elves are testing negative.
"We're not going to take any chances. We're all going to mask up. We're all going to wash out hands and we're all going to stay six feet apart," he said.
It's pretty funny to think about her lining up this homily from Santa while she is pushing for a statewide mask mandate.
"There is no question COVID-19 has created a lot of hardships in 2020. And it's not my fault, it's not the legislature's fault. The legislature needs to pass legislation to protect public health, including a mandate that we wear masks until the majority of us have had this vaccine.
I know that there is bipartisan support for that action. I'd love to see the legislature take action. These are crucial things we can do to protect our people and our businesses here in Michigan," she said.
This is as predictable as it gets. All of the cowardly governors who could not successfully force masks and lockdowns onto people before are going to try again now.
Biden being elected has emboldened them, big time. Whitmer's speech is so ridiculous, we could hardly believe our eyes. This woman is brainwashing the youth of America into believing her nonsense and there is nothing we can do about it. Now that Sleepy Joe is about to regain power, she's going to feel as if she could do anything she wants.
Whitmer and like-minded governors have been operating under this mentality all year long. They are fine with all of these rules because they are not going to bother to adhere to them anyway. How can you even reason with someone who is willing to trot out Santa Claus to tell the children all about the necessity of mask-wearing?
This is the same woman who tried to keep people from traveling to their own lake houses, just so she could go to hers. People would probably be a lot more willing to go along with what is being said right now if they knew that their leaders were actually in the struggle with them.
They already know that this is not the case, hence the skepticism.
We have all seen the same routine over and over again. The Democratic governor comes out and offers platitudes about how we all need to stick together.
From there, everyone is told to stay inside and wear masks if they decide to go out. This is all well and good until the governor in question inevitably ends up exposing their own hypocrisy.
At least there is a vaccine on the horizon. Once the holidays have passed, it will be harder and harder for leaders to start firing off these terrible opinions.
We are sure that couples will be told to stay out of restaurants on Valentine's Day but that shouldn't be a big deal. Most of the casual dining spots are sure to be shut down.
Hopefully, by the time Easter rolls around, a larger portion of the nation is vaccinated. This will allow us to resume our normal holiday schedules, without worrying about running afoul of Democratic governors like Whitmer.
Let's all write to our socially distanced Santa Claus and tell him that we would like some normalcy for Christmas next year. It's not a big ask!
Baseball Legend Curt Schilling Says AIG Cancelled Insurance Because He's Conservative — But Here's Who They Will Insure
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Timeless Gift
We at Zed Photography, love photographing Christenings/ Baptisms. It's such an emotional, loving, treasured day for family & friends. It's a milestone that takes an instant out of time by capturing your child's once in a life time "right of passage". Creativity and sensitivity is our approach to capturing these moments forever. We love celebrating this joyous gathering, recording this milestone and sharing it with family and loved ones. It's a connection like no other. We can't speak on behalf of other photographers but it's like we become one with the family.
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Silver with Distinction and three Silver Awards, portrait category,
Epson AIPP Victorian Professional Photographer of the year.
Silver with Distinction and Silver Award, portrait category,
Canon AIPP Australian Professional Photographer of the Year


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Review: Tarzan - The Jungle Warrior by Andy Briggs
When a baby gorilla is snatched from its family by the world's most infamous hunter, Tarzan will stop at nothing to track him down - crossing the wild jungle and hostile African savannah to bring him to justice.
Meanwhile, Jane is trying to learn more about Tarzan's past, and must decide whether reuniting him with his lost Greystoke family is the right thing to do. But Robbie has ideas of his own. He has formed a plan that will get rid of Tarzan for good, and keep the secrets of his own past safe.
Last year I wrote a glowing review for Tarzan: The Greystoke Legacy, Andy Briggs' superb reboot featuring Edgar Rice Burroughs' iconic character. Since then I have been eagerly awaiting the next book in the series, and pretty much dropped everything when a copy arrived through my letterbox. I am happy to report that not only has Andy Briggs produced another thrilling adventure story that young readers will adore, it is also possibly even better than its predecessor.
The book opens with Nikolas Rokoff, the greatest hunter in the world, receiving a commission to venture into the Congo to bring back a gorilla. So begins a white knuckle ride of an adventure that sees Tarzan, Jane and Robbie risking life and limb as they travel across Africa in pursuit of Rokoff. This is action/adventure writing at its very best, with scene after scene after scene that are just begging to be put on the big screen.
Whilst the first book was a great introduction to the main character for a 21st Century audience, it also introduced us to Jane and Robbie, both of whom are not particularly happy with the hand they have been dealt in life. In this book we see their characters developed even further, with Jane becoming tougher and more independent (in a good way), and Robbie struggling with his conscience, especially with regards to Tarzan and the avaricious plans he and Clark are making as they aim to prove to the Greystokes that the legitimate heir to the estate is alive and kicking.
Andy Briggs pulls no punches with his legendary king of the jungle, and the story certainly hasn't been sanitised for the modern audience. When he needs to be, Tarzan is a brutal and unmerciful killer, but in his mind every one of his actions is justified if it involves the protection of his home, and more importantly its animals, the only family Tarzan has ever known. Whilst we saw a few moments of Tarzan's explosive fury at civilised man's wilful destruction of his jungle habitat and its fauna in the first book, in this sequel they happen far more frequently as he battles against poachers who think nothing of slaughtering elephants for ivory, or capturing animals for wealthy collectors. Young readers are left to decide for themselves whether the end justifies his means, and the book is a thought-provoking story that could make a great starting point for discussions about poaching and other environmental issues.
As I said in my review of The Greystoke Legacy, I am no expert on the original Tarzan books, although I know a number of people who are big fans of both ERB's series and that first book by Andy Briggs. They tell me that although they had their doubts about the character being updated for a modern story, they also felt that Briggs and got the king of the jungle nailed perfectly in their minds. As I was discussing this book with one of them I mentioned Rokoff's character and I was told that Andy Briggs certainly knew he stuff. A quick google later and I found out that Rokoff, and his assistant Alexis Paulvitch who also appears in The Jungle Warrior, are characters who both feature in the original stories of Edgar Rice Burroughs, as does D'Arnot, the man who taught Tarzan to speak English.
I flew through this book and I think young readers will do exactly the same, as the plot races along at a fantastic pace as the trio pursue Rokoff across a handful of African countries. It is the kind of book that will also have readers vocally cheering on the jungle hero, especially during the many superbly written fight sequences. Although the main plot line of the story is brought to a satisfying conclusion, Andy Briggs pulls something of a fast one and the final paragraph will have readers clamouring for the next title in the series.
Tarzan: The Jungle Warrior is due to be published on 12th July and my thanks go to the good people at Faber for sending me a copy to review. Come back here on 13th July for a guest post from Andy Briggs, as part of the Tarzan: The Jungle Warrior blog tour.
Posted by BookZone at 6/26/2012 08:30:00 pm
have you ever met rick
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Mitchell Ready to Step Up
By: TheSabre.com | October 12, 2012
Akil Mitchell can be an effective offensive player, but has to let the game come to him.
Akil Mitchell has some pretty big shoes to fill this season. With the departure of senior post leaders Assane Sene and Mike Scott, and the transfer of James Johnson , Mitchell now becomes the only true veteran in the post. While Coach Tony Bennett suggests offense will now come from a "committee" of players, there's no doubt Mitchell will be called upon to do a lot of the dirty work in the paint (i.e. rebounding and defense).
Mitchell averaged 4.1 points and 4.4 rebounds per game last year in 22 minutes. While the point average is low, don't be fooled. Mitchell can score when needed and has been working on improving his face-up mid-range shot to help the transition from Scott's team-leading 18 points per game last season. Mitchell says he'd like to be a double-double type of performer, much like Scott in his final two seasons. And while that seems a bit optimistic, senior point guard Jontel Evans thinks Mitchell has the potential to be that kind of player.
"I definitely do. He showcased that in Europe", says Evans. "There was one game he had 20 points and 16 rebounds. He just has to do the things he's capable of doing, like rebounding, catch and shoot 15 feet from the basket, and running the floor. Once he's locked in on those categories, he's a tough player to match up with."
Coach Tony Bennett hasn't assigned any point or rebounding goals for Mitchell, but did offer this.
"Akil had a nice summer for us. He showed a little more production", said Coach Bennett. "Akil just has to be Akil. At the end of the year he started playing some good basketball for us. He was productive with offensive rebounds and finishing plays. And he has worked hard to develop some more work on his shots, some more moves, whether he's facing the basket, off the lane, or just little things. Just the
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Be on the lookout for our construction crew as we continue to bury NEW Fiber Optic Cable. This new cable is allowing us to provide faster, more reliable service to our customers. Also Provide Service to in Places we were unable to before.
So if you see these guys give them a wave!
© 2015 | Community Telephone Company, Inc./COMCELL, Windthorst TX. All rights reserved.


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Find out more about our Species at Risk
Pacific Cuttrout Trout
Cutthrout Trout: Onchorynchus clarkii clarkii spp.
Species: Coastal Cut-throat Trout – Onchorynchus clarkii clarkii spp.
B.C. Status: Blue
Coastal cutthroat trout are a subspecies of the cutthroat trout. All cutthroat trout are the same genus as Pacific Salmon. They too are salmonids although they have a different spawning and life cycle from salmon. Cutthroat trout stay close to the shore and do not necessarily "run" as do the salmon.
There are two varieties of the coastal cutthroat trout, resident (freshwater) and sea-run. Depending on the circumstances, some coastal cutthroat will swim their way to the ocean to spend part of their life in the salty waters, while others will begin and complete their lifecycle in freshwater bodies. Other than the salinity, both varieties of coastal cutthroat have the same habitat requirements.
For a healthy coastal cutthroat population, clean and clear water with plenty of oxygen is essential. Coastal cutthroat trout are sensitive fish and wherever they are found, they indicate a healthy ecosystem. As sensitive fish, they need vegetation around the bodies of water in which they live. Vegetation provides shelter from the sun, habitat for their prey (insects, invertebrates and small fish) and also prevents streamside erosion.
Pools created by large debris and/or natural pools such as lagoons also create shelter for the coastal cutthroat trout to live.
Stream flow is very important for these fish during their early development. They require a consistent and specific water flow (velocity). Too strong of a flow may degrade the channel and can wash away young fish to the sea too early, while too slow a flow can increase competition with other fish.
The spawning cycle of the coastal cutthroat trout is different than that of other salmonids. They can spawn repeatedly (they do not die after spawning) between December and May, so long as they have a suitable nesting spot with clean gravel and water. The eggs are laid in the gravel, and after about 7 weeks emerge as little fry. For two to five years they remain in the freshwater body in which they are reared. Once they have matured into smolts they begin their migration to other bodies of water, be it ocean or fresh water. After about a year, they return to spawn.
Coastal cutthroat trout are very important to our aquatic ecosystems, they help balance and connect the coastal and freshwater food web, they are both predator and prey. They feed and nourish many predator species including great blue herons, bears, river otters, osprey, mink, adult salmon, seals and humans!
The coastal cutthroat trout is a species of special concern. A decline in their population is indicative of a change in their habitat. Pollution, degraded water quality, change in water flow, erosion, excess sediment, etc. are all of concern. As sensitive fish, there are many activities in which humans can contribute to changes in their population, both positively and negatively.
Identification – what to look for?
Sleek fish with blueish-green backs
Silver sides
Many spots
Reddish/orange under jaw
Jaw is long and extends further than their eyes
Can grow as big as 10–18 inches and older fish can be over 20 inches in healthy ecosystems
Where are they found?
Along the coast, close to the shore in estuaries, lagoons and in freshwater streams, lakes and beaver ponds
Around the aquatic vegetation in water bodies with insects
They love little hiding spaces and shelter from the sun, so can be found around logs and fallen debris and vegetation in water
In year-round water flow, which isn't too fast, nor too slow
Sea-run coastal cutthroat love shelter in lagoons and estuary pools, typically among the eelgrass
On Cortes Island, they are found in Hague and Gunflint Lakes
Cool facts!
It is believed that all subspecies of cutthroat trout (freshwater fish) evolved from the coastal cutthroat trout species (marine fish)
Sea-run and resident cutthroat trout can successfully reproduce together as they may end up in the same breeding spot
Typically both the sea-run and the resident cutthroat trout stay within 50 miles of the stream in which they hatched in
Coastal cutthroat trout do not die after they spawn, in fact it is believed that they may skip a year of spawning
The amount of eggs laid depends on the size of the fish, anywhere from 100 to 600 eggs
Some resident cutthroat trout can live for over 15 years! Sea-run can live for around 10 years
Government of Alaska (PDF)
South Coast Conservation Program
Western Toad
Coastal Cutthroat Trout
Northern Pygmy Owl
Threaded Vertigo
Big Eared Bat
Pacific Sideband Snail
Sooty Grouse
Northern Red-Legged Frog
Join the FOCI family
Become a Friends of Cortes Island member and support the work that we're doing in the community to help look after our beautiful island.


This is scheduled for one of the upcoming book chats at noontime. Hope you will stop in and give your thoughts!
Thank you for a wonderful review Jaime! I'm glad you enjoyed it, and I'm working on the second one right now 😉 It's a sequel, titled "Shattered", so keep an eye out for it over the next few months!
Hey this is a great Review. I was sold on the first sentence! Sounds like a good story.


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35 Inspirational Mila Kunis Quotes On Success
Milena Markovna Kunis is an American actress. In 1991, at the age of 7, she moved from Soviet Ukraine to the United States with her family. After being enrolled in acting classes as an after-school activity, she was soon discovered by an agent. She appeared in several television series and commercials, before landing her first significant role at age 14, playing Jackie Burkhart on the television series That '70s Show (1998–2006). Since 1999, she has voiced Meg Griffin on the animated series Family Guy. May these Mila Kunis Quotes On Success inspire you to take action so that you may live your dreams.
1. "My goal in life is to enjoy what I do, and never to look back and say I wish I would have done that, and to go to UCLA, and to become someone great in life!" Mila Kunis
2. "You want to be honest with a character and play it truthfully, and you want to be genuine with your character." Mila Kunis
3. "I stand by every movie that I did. I don't regret any decision I made." Mila Kunis
4. "I wanted to just surround myself with people who I think are better than I am, whether they're actors or directors or producers, so that I could learn from them." Mila Kunis
5. "Always have a backup plan." Mila Kunis
6. "I honestly think being single's great. Being in a relationship's great. It's all about the timing." Mila Kunis
7. "Whether you know who Denzel Washington is or you don't, when he walks into the room, you're going to pay attention, because he's just such a powerful man." Mila Kunis
8. "It's not the most normal life in the world, but I screw up plenty of times to be a normal teenager." Mila Kunis
9. "I think there will always be a double standard between males and females, so I think that an actress is more likely to protect her public persona, so to speak, than an actor would be." Mila Kunis
10. "It's fun working on the set. I usually work about 10 and a half hours a day, and I also study about five of those hours. It can be tiring, but it's fun!" Mila Kunis
11. "I grew up incredibly poor and went to school and had a very average upbringing." Mila Kunis
12. "The thing about ballet that I never knew about is that it's one of the most excruciating sports that I've ever been a part of. I say sports because they train constantly, every single day." Mila Kunis
13. "I definitely hope to attend UCLA in a year, and major in business." Mila Kunis
14. "I went to college because I felt like I was supposed to. I graduated from public high school and I did all the things that I was supposed to do." Mila Kunis
15. "I feel like every role you take, there's a part of you that obviously feels like you can do it. I don't know if perfect is the right word because I don't believe in perfection. I don't think it exists." Mila Kunis
16. "I think that an actor is more likely to be forgiven in the public's eye than an actress." Mila Kunis
17. "I love playing different characters and I love doing fun things and I love to entertain people, whether that be in a comedy or a drama. If I get you to laugh or I get you to cry I'm super stoked, as morbid as that might sound." Mila Kunis
18. "My dad heard of a studio on the radio, and it was advertised as a place for kids to meet kids, and it was actually a studio, and that's where I met my manager and agent." Mila Kunis
19. "Confidence, not cockiness. Knowing who you are is confidence. Cockiness is knowing who you are and pushing it down everyone's throat." Mila Kunis
20. "Sadly, in any industry and in any work-related environment, females always strive to achieve a certain amount of perfection, whether that be skinny or pretty. It's a constant, in our society." Mila Kunis
21. "I think that certain things are funny and certain things are okay to make fun of – including myself." Mila Kunis
22. "My mom and my dad wanted my brother and I to have a better life, you know, better education, better jobs. It was probably harder, much, much harder, for my parents. When you're a kid, you can learn a language much more easily; I learned English in less than a year." Mila Kunis
23. "Teens are dealing with the same problems now in the '90s as they did back in the '70s, the only real difference is the clothes we wear!" Mila Kunis
24. "I'm not boring to be around. Something will always happen." Mila Kunis
25. "I had a normal upbringing and went to public school. If I ever, even for a second, started getting a big head, I was brought back to reality pretty quickly. I was working full time and still had to fight for a cell phone." Mila Kunis
26. "I am very much a creature of habit, and I have no life consistency. None." Mila Kunis
27. "I think that when a person is insecure about who they are or who they want to be, then it translates on screen, and the choices they make are all about perception." Mila Kunis
28. "It is difficult because the school I go to, my friends do not attend." Mila Kunis
29. "I am in the position where I don't have to work for the sake of working, so I'm very lucky, in a sense. So, I can always sit back and wait for a project that I respond to, that I want to do." Mila Kunis
30. "I've definitely grown apart from a lot of my friends. Some of them don't understand the schedule, and it's not that I don't want to talk to them, it's that sometimes I am really busy and can't get back to them." Mila Kunis
31. "I enjoy living life and I enjoy going to different restaurants and eating my way through a country and going to different museums and learning about different cultures." Mila Kunis
32. "I love swimming, tennis, and I am taking up golf. I am not serious about it, I just go to the range and practice. Other than that, I enjoy going to the movies and hanging out with my friends." Mila Kunis
33. "I don't think it's true that blondes have more fun. Trust me, it is not true!" Mila Kunis
34. "People have interpretations of what you're supposed to be like. If you're unattractive and overweight, you must have a great personality. If you're attractive, then you must not be the nicest person. People are always taken aback that I'm easygoing but not necessarily stupid." Mila Kunis
35. "It's not having what you want. It's wanting what you've got." Mila Kunis
I hope you enjoyed these Mila Kunis Quotes On Success. Do let us know which one was your favorite in the comments section below.
Check Out Mila Kunis Spent Her Honeymoon In An RV Park With Ashton Kutcher's Parents:
35 Safety Quotes On Success
35 Inspirational Upton Sinclair Quotes On Success


to make the connection between art and education in museum work and provided her with the nexus to combine these interests into a career.
Back at W&J, Schmidt continued to guide Mastromarino by enrolling her in a 300 level art history course, typically taken by seniors, when she was only a sophomore. The class solidified her interest in museum work and led her to a semester abroad in Florence studying art. After graduation, she earned a master's degree in museum studies from Johns Hopkins University.
Her current job as the traveling exhibits manager at the Children's Museum in downtown Pittsburgh allows her to combine the aesthetics of exhibit design with a focus on educating the public. Her job duties include assisting in the creation of new exhibits, marketing existing assets, brand management, working with partners such as The Eric Carle Museum of Picture Book Art and Fred Rogers Productions, and ensuring exhibit quality from site to site.
Mastromarino started at the museum as an unpaid intern in 2011 and rose through the ranks from a part-time museum associate to a full-time manager. Prior to Mastromarino's arrival, the museum lacked a strong focus on traveling exhibits, and only traveled one exhibit from 2007 to 2014.
"XOXO: An Exhibit About Love & Forgiveness" premiered in Pittsburgh in 2014 and now tours the country. The exhibit centers on teaching visitors about love and forgiveness through interactive experiences that focus on communication. The foreground of the photo showcases "Tone Phones," which allow visitors to visualize their voices on the projected surface showing them that it's not what you say, it's how you say it. XOXO has traveled to a variety of museums including the Muhammad Ali Center and the Canadian Museum of Human Rights.
After grant funding allowed the museum to create a new traveling exhibit, "XOXO: An Exhibit About Love & Forgiveness," it decided to expand the traveling exhibit program. As a result of this decision, the museum launched its Business Development Initiative in 2014 with Mastromarino in the role of the business development coordinator. As the initiative grew, she took on the role of traveling exhibits manager in 2016. The museum has seen success with its traveling exhibits, and produced five new exhibits, one per year, between 2014 and 2018.
The Children's Museum of Pittsburgh is one of less than 10 producers of children's traveling exhibits nationwide. Organizations across the country pay to house these exhibits in their spaces for certain periods of time, with the revenue generated coming back to the museum. The museum also leverages its expertise to offer consulting services on exhibit design and marketing to like institutions.
Each exhibit has a 10-year lifespan and is displayed at two or three locations per year, meaning approximately three million people will interact with an exhibit produced by Mastromarino and the 10-person exhibits team over its lifetime.
A wide assortment of considerations goes into determining the factors of an exhibit.
In addition, the components of the exhibit must travel well, as it will be loaded and unloaded onto trucks and set up in a variety of different spaces over its lifespan.
"I have to deal a lot with 53-foot tractor trailers, which I never thought I would be doing," she said.
Exhibit prototypes go through a testing period with staff evaluators and researchers to determine what is needed to provide the best visitor experience.
Finalized exhibits debut at the museum in Pittsburgh for six months before hitting the road. This gives museum staff additional time to create the materials needed to promote the exhibit, as well as identifying any problems that may arise once it is open to the public.
Once the exhibits begin to travel, Mastromarino manages them from afar, following along with the reaction they receive in the press and on social media. The Very Eric Carle exhibit, most recently on display in Bettendorf, Iowa, received a mention in USA Today's travel section as one of the top ten museum exhibits in the country to see this summer.
While her exhibits travel from coast to coast, Mastromarino and her husband Alex Patterson '11, chose to stay close to the friends and connections they made during their time at W&J and have settled in Pittsburgh.
Mastromarino came to Washington from Reading, Pa., to be a part of the field hockey team and have a small college experience. She met Patterson, a football player from Cincinnati, through athletics at Cameron Stadium.
The team-oriented environment that drew Mastromarino to W&J allowed her to make close connections and find her passion, leading her to a career that capitalizes on the thriving arts scene of nearby Pittsburgh.
Find out if the Children's Museum exhibits are traveling to a city near you: pittsburghkidsdesign.org/traveling-exhibits.


Foraging : The kite will forage over open lands.
Nesting : Generally <600m Red kites require trees for nesting, although the Cape Verde race of the red kite has reportedly been found to nest on cliffs occasionally.
Nests : Red kites build large stick nests. Nests are lined with sheep's wool. Nests are often decorated with fresh greenery or pieces of rubbish.
Red Kites do not have strong habitat preferences. Over their European range they tend to avoid extremes of climate, hence they're restricted distribution. Kites hunt over open landscapes. In many areas they are closely associated with farmland. The mixed landscape that man has created throughout much of Europe has greatly benefited the kite. An undulating landscape more readily provides thermals for the kites to soar on than a flat one. Locally kites may prefer rolling terrain or the foothills of mountains because of the thermals. Large areas of forest are generally avoided except for nesting or roosting in. Small copses can be utilised for hunting.


text:
\section{Introduction}

The concept of wobbling motion in atomic nuclei was originally
introduced by Bohr and Mottelson in the 1970s~\cite{Bohr75}. It is described as the small amplitude harmonic oscillations of the total angular
momentum with respect to the principal axis having the
largest moment of inertia (MOI)~\cite{Bohr75}. With increasing angular momentum components along the two axes with smaller MOI, it
excites a family of $\Delta I=2$ rotational bands corresponding to increasing phonon quanta $n$.
These bands are connected with enhanced collective $\Delta I=1$ $E2$ transitions. The pioneering work of  the
microscopic description on wobbling motion  was introduced by Marshalek~\cite{Marshalek79}.
It was first proposed to appear in triaxial even-even nuclei with
zero quasiparticle configuration~\cite{Bohr75}, while the corresponding experimental evidence is still scarce.
For instance, the $\gamma$ bands in $^{112}$Ru were interpreted as a possible evidence~\cite{Ru112}, but no interband electromagnetic transition rates were reported.

Instead, wobbling bands have been widely reported in odd-mass nuclei.
It was first suggested in the triaxial strongly deformed bands of $^{163}$Lu~\cite{Lu1631,Lu1632}
and later in other neighboring nuclei $^{161}$Lu~\cite{Lu161}, $^{165}$Lu~\cite{Lu165}, $^{167}$Lu~\cite{Lu167}, $^{167}$Ta~\cite{Ta167}.
Then, experimental evidences of wobbling motion was also reported in other normal deformed nuclei: $^{105}$Pd~\cite{Pd105}, $^{130}$Ba~\cite{Ba130,Ba1302}, $^{133}$Ba~\cite{Ba133}, $^{135}$Pr~\cite{Pr135,Pr1352}, and $^{183}$Au~\cite{Au183}, where the wobbling energies decrease with increasing spin contrary to the theoretical expectations in Ref.~\cite{Bohr75}. Frauendorf and D\"{o}nau~\cite{Frauendorf14} interpreted this behavior as the odd particle aligned perpendicular to the principal axis with the
largest MOI, which  was defined as transverse wobbling (TW). In addition,
$^{127}$Xe~\cite{Xe127}, $^{133}$La~\cite{La133} and $^{187}$Au~\cite{Au187} exhibit longitudinal wobbling (LW), where the odd particle aligned parallel to the principal axis with the
largest MOI. For the ideal TW (LW), the total angular momentum is aligned along the short (intermediate) axis in the yrast band. With one phonon excitation, the precession of total angular momentum occurs with respect to the short (intermediate) axis~\cite{Frauendorf14,Au187}, which is presented
pictorially in Figs.~\ref{fig:picture}(a) and \ref{fig:picture}(c). Very recently, an experiment for $^{135}$Pr provided the crucial evidence against the proposed wobbling nature~\cite{Pr135tilted}, which questioned the interpretation of wobbling.

On the theoretical side, the wobbling excitation got extensive descriptions with the particle rotor model (PRM)~\cite{Frauendorf14,Hamamoto02,
Hamamoto2003PRC, Hagemann04, Streck18,Broocks21,CQB19} and
its approximation solutions~\cite{Tanabe08,Tanabe10,Tanabe17, Budaca2018PRC,Budaca2021, Raduta2018, Raduta2020JPG, Raduta2020PRC,Raduta2021,Lawrie20}.
In addition,
the random phase approximation~\cite{Matsuzaki02, Matsuzaki2003PRC,Matsuzaki2004PRC, Matsuzaki2004PRC_v1,Shimizu2005PRC,Shimizu2008PRC,Shoji09, Frauendorf2015PRC, Nakatsukasa16},
the angular momentum projection  method~\cite{Pr1352,Ba1302,Shimada18},
and the collective Hamiltonian method~\cite{CHENQB14, CHENQB16,WXH18} are used to discuss this issue.
However, it should be noted that there are still increasingly loud debates on the TW in odd-mass nuclei.
Reference~\cite{Tanabe17} used an approximation to the PRM to study the stability of TW and concluded there is an absence of the wobbling mode around the axis with medium MOI.
This issue was
further discussed~\cite{Budaca2018PRC,Frauendorf182,Tanabe18}.
Furthermore, an alternative mode for the candidate wobbling band was proposed in Ref.~\cite{Lawrie20}, $i.e.$, a precession of the total angular momentum around a certain tilt axis (called tilted precession bands), which is presented in Fig.~\ref{fig:picture}(b).

Whether the stable TW exist in odd-mass nuclei is still an open question. In this paper, we took $^{105}$Pd as an example and made an attempt to clarify some disputes about TW motion. Recently,
two bands built on $\nu h_{11/2}$ configuration in $^{105}$Pd had been suggested as TW due to
the $\Delta I=1$ transitions between them with a predominant $E2$ component and
the decreasing wobbling energy with increasing spin~\cite{Pd105}.
The behavior of the wobbling bands in $^{105}$Pd has been reinvestigated by the quantum PRM. The different parameter sets of MOI will be searched to reproduce the experimental data. The corresponding rotational modes will be analyzed in detail in terms of the azimuthal plot of angular momentum. Consequently, the picture of TW will be examined.

\section{Theoretical Framework}

The Hamiltonian of the particle rotor model can be expressed as~\cite{Bohr75,Ring}
\begin{eqnarray}
\hat{H}=\hat{H}_\textrm{{coll}}+\hat{H}_\textrm{{intr}}
\end{eqnarray}
with the collective Hamiltonian
\begin{eqnarray}
\begin{aligned}
\hat{H}_\textrm{{coll}}&=\sum_{k=1}^{3}\frac{\hat{R}_{k}^{2}}{2{\cal J}_{k}}=\sum_{k=1}^{3}\frac{(\hat{I}_{k}-\hat{j}_{k})^{2}}{2{\cal J}_{k}}\\
&=\sum_{k=1}^{3}\frac{\hat{I}_{k}^{2}}{2{\cal J}_{k}}+\frac{\hat{j}_{k}^{2}}{2{\cal J}_{k}}-\frac{\hat{I}_{k}\hat{j}_{k}}{{\cal J}_{k}},
\end{aligned}
\end{eqnarray}
where $k=1,2,3$  denotes the three principal axes of the body-fixed frame corresponding to the intermediate ($m$), short ($s$), and long ($l$) axis for $0^{\circ}<\gamma<60^{\circ}$, respectively.  Here $\hat{R}_{k}$, $\hat{I}_{k}$, and $\hat{j}_{k}$, respectively, denote the angular momentum operators for the core and nucleus as well as the valence nucleon.
The parameters ${\cal J}_{k}$ are the MOI for three principal axes.

Two models of MOI are usually taken in the study of wobbling~\cite{Tanabe17,Tanabe18}, $i.e.$, the hydrodynamical MOI:
\begin{eqnarray}
{\cal J}_{k}={\cal J}_0 \sin ^{2}(\gamma-\frac{2 k \pi}{3})
\end{eqnarray}
and the rigid-body MOI:
\begin{eqnarray}
{\cal J}_{k}= \frac{{\cal J}_0}{1+(\frac{5}{16\pi})^{1/2} \beta }[1-(\frac{5}{4\pi})^{1/2}\beta \cos (\gamma+\frac{2 k \pi}{3})].
\end{eqnarray}
The above expressions are different from the standard convention of $k = x, y, z$, in which the sign of
$\gamma$ is meaningful~\cite{Hamamoto02,Ring}.

The intrinsic Hamiltonian $\hat{H}_\textrm{{intr}}$ describes a single valence nucleon in a high-$j$ shell
\begin{eqnarray}
\hat{H}_\textrm{{intr}}=\pm\frac{1}{2} C\left\{\cos \gamma\left(j_{3}^{2}-\frac{j(j+1)}{3}\right)+\frac{\sin \gamma}{2 \sqrt{3}}\left(j_{+}^{2}+j_{-}^{2}\right)\right\},
\end{eqnarray}
where $\pm$ refers to a particle or a hole state and the coefficient $C$ is proportional to the quadrupole deformation parameter $\beta$~\cite{Qi09}. Differing from the frozen approximation proposed in Ref.~\cite{Frauendorf14}, we present our calculations with free odd-particle angular momentum.

To obtain the PRM solutions, the total Hamiltonian must be diagonalized in a complete basis space, which couples the rotation of the core with the intrinsic wave function of a valence nucleon. When pairing correlations are neglected, one can construct the so-called strong coupling basis~\cite{Ring,Qi09},
\begin{eqnarray}
|I M K j \Omega +\rangle= \sqrt{\frac{2 I+1}{16 \pi^{2}}}\left[D_{M K}^{I}|j \Omega\rangle +(-1)^{I-j} D^{I}_{M-K}|j-\Omega\rangle\right],
\end{eqnarray}
where $I$ denotes the total angular momentum of the odd-mass nuclei and $K$ refers to the projection onto the 3-axis of the intrinsic frame. Furthermore, $\Omega$ is the 3-axis component of the valence nucleon angular momentum $j$ in the intrinsic frame. Under the requirement of the $D_{2}$
symmetry of a triaxial nucleus,
$K-\Omega$ need to be an even integer. The matrix elements of total Hamiltonian can be evaluated in this basis, and the diagonalization gives eigenenergies and eigenstates for the PRM Hamiltonian. The wave function of PRM can be expressed as
\begin{eqnarray}\label{PRMfun}
|I M \rangle = \sum\limits_{K,\Omega} C_{IK j\Omega} |I M K j \Omega +\rangle.
\end{eqnarray}

The reduced  electric quadrupole transition probabilities are calculated by the operator
\begin{eqnarray}
{\hat{\cal{M}}}(E2, \mu) =\sqrt{\frac{5}{16\pi}}\hat{Q}_{2\mu}
\end{eqnarray}
with the obtained wave functions. The quadrupole moments
in the laboratory frame ($\hat{Q}_{2\mu}$) and the intrinsic
system ($\hat{Q}'_{2\mu}$) are connected by the relation
\begin{eqnarray}\label{Q0}
\begin{aligned}
\hat{Q}_{2\mu}&=\mathcal{D}_{\mu 0}^{2 *} \hat{Q}_{20}^{\prime}
+\left(\mathcal{D}_{\mu 2}^{2 *}+\mathcal{D}_{\mu -2}^{2 *}\right) \hat{Q}_{22}^{\prime}\\
&=\mathcal{D}_{\mu 0}^{2 *} Q\cos \gamma
+\left(\mathcal{D}_{\mu 2}^{2 *}+\mathcal{D}_{\mu -2}^{2 *}\right) \frac{1}{\sqrt{2}}Q\sin \gamma.
\end{aligned}
\end{eqnarray}

For $M1$ transitions, the magnetic dipole transition operator can be written as
\begin{eqnarray}
 \hat{\cal{M}} (M1,\mu) = \sqrt{\frac{3}{4\pi}} \frac{e\hbar}{2Mc}
 [(g_j-g_R)\hat{j}_{\mu}],
\end{eqnarray}
where $g_j$ and $g_{R}$ are, respectively, the effective gyromagnetic ratios for valence nucleon and the collective core, and $\hat{j}_{\mu}$ denotes the spherical tensor in the laboratory frame.

Using wave functions obtained from the PRM, one can calculate the
expectation values of the core angular momentum as
\begin{eqnarray}
\langle R_{k}^2 \rangle^{1/2} & = \langle I M |(\hat{I_{k}}-\hat{j_{k}})^{2}|I M \rangle^{1/2}.
\end{eqnarray}

To illustrate clearly the angular-momentum geometry,  the probability distribution of the total angular momentum on the $(\theta, \varphi)$
plane, $i.e.$, azimuthal plot~\cite{Streck18,CFQ17,CQB18,CQB19}, is calculated.
Here $(\theta, \varphi)$ are the orientation angles of the angular-momentum
vector $\textit{\textbf{I}}$ (expectation value with $M = I$ ) with
respect to the intrinsic frame. The polar angle $\theta$ is the
angle between $\textit{\textbf{I}}$ and the $l$ axis, and the
azimuthal angle $\varphi$ is the angle between the projection of $\textit{\textbf{I}}$ on
the $sm$ plane and the $m$ axis. The
profile is calculated as~\cite{Streck18,Qi21}
\begin{eqnarray}\label{APlot}
\begin{aligned}
\mathcal{P}^{(\nu)}(\theta, \varphi)&=\langle I, \theta \varphi \mid I I \nu\rangle^{2}\\
&=\frac{2I+1}{8\pi}\sum\limits_{K K^{\prime}} D_{K I}^{I *}(\theta, \varphi, 0)
\rho_{KK'}^{(\nu)} D_{K^{\prime} I}^{I}(\theta, \varphi, 0),
\end{aligned}
\end{eqnarray}
where $\rho_{KK'}^{(\nu)}=\sum\limits_{\Omega}C_{IKj\Omega}^{(\nu)}C_{IK'j\Omega}^{(\nu)}$ with the expansion coefficients $C_{IKj\Omega}^{(\nu)}$ in Eq.~(\ref{PRMfun}).

Here we further calculate the profile for the valence nucleon angular momentum~\cite{Frauendorf20},
\begin{eqnarray}
\begin{aligned}
\mathcal{P}^{(\nu)}(\theta, \varphi)&=\langle j, \theta \varphi \mid j j\nu\rangle^{2}\\
&=\frac{2j+1}{8\pi}\sum\limits_{\Omega \Omega^{\prime}} D_{\Omega j}^{j *}(\theta, \varphi, 0)
\rho_{\Omega \Omega^{\prime}}^{(\nu)} D_{\Omega^{\prime}j}^{j}(\theta, \varphi, 0)
\end{aligned}
\end{eqnarray}
with the density matrix
$\rho_{\Omega\Omega^{\prime}}^{(\nu)}=\sum\limits_{K} C_{I K j\Omega}^{(\nu)} C_{I K j\Omega^{\prime}}^{(\nu)}$.

Both the profiles $\mathcal{P}^{(\nu)}(\theta, \varphi)$ fulfill the normalization condition
$$\int_{0}^{\pi} d \theta \sin \theta \int_{0}^{2 \pi} d \varphi \mathcal{P}^{(\nu)}(\theta, \varphi)=1.$$

\section{Results and Discussion}

\subsection{Description of the data}

Following Ref.~\cite{Pd105}, the configuration $\nu (1h_{11/2})^{1}$
with a triaxial shape of $\beta=0.27$ and $\gamma=25^{\circ}$ for $^{105}$Pd is taken in our calculation.
The triaxial rotor is parametrized by three angular-momentum-dependent MOI
 ${\cal J}_{k}=a_{k}\sqrt{1+bI(I+1)}$~\cite{Pd105}.
Both of hydrodynamical and rigid MOI with such triaxial shape are ${\cal J}_{1}>{\cal J}_{2}>{\cal J}_{3}$, $i.e.$, ${\cal J}_{m}>{\cal J}_{s}>{\cal J}_{l}$. In the following discussion, the three principal axes  are marked by the suffixes $m$,  $s$, and $l$  for  convenience.
For $\gamma=25^{\circ}$, the ratio between the MOI at intermediate and short axis ${\cal J}_{m}/{\cal J}_{s}$ is approximately equal to $1:0.9$ for a rigid-body MOI and $1:0.3$ for a hydrodynamical MOI.
Four typical sets of parameters are adopted and listed in Table~\ref{tab:Pd105MOIset}, in which ${\cal J}_{m}/{\cal J}_{s}$ takes values of  $1:0.9$~(A), $1:0.7$~(B), $1:0.5$~(C), and $1:0.3$~(D), respectively. The corresponding parameters $a_m$ and $b$
are determined by fitting the energy spectra of yrast band A and yrare band B in $^{105}$Pd.
In Ref.~\cite{Pd105}, ${\cal J}_{m}/{\cal J}_{s}=1:0.63$ with $b=0.023$ was adopted, which is between the ratio of the parameter sets (B) and (C).
${\cal J}_{l}$ is determined by fitting the energy difference between yrast and yrare band, and such an energy difference is found to be smaller for the bigger value of ${\cal J}_{l}$.

For the electromagnetic transitions, we used the intrinsic
quadrupole moments $Q=(3/\sqrt{5\pi})R_{0}^{2}Z\beta=3.0$ eb,
the gyromagnetic ratios $g_{R}=Z/A=0.438$ for the rotor and $g_{\nu }(h_{11/2})=-0.209$ for the neutron.
Note that a quenching factor of $0.36$ for $g$ is introduced in our calculation same as Ref.~\cite{Pd105}. This is due to the scissor mode which is mixed with the wobbling motion and cannot be considered in the PRM calculations~\cite{Pd105}.

The calculated energy spectra, wobbling energies and reduced transition probability ratios [$i.e.$, $B(E2)_{\textrm{out}}/B(E2)_{\textrm{in}}$ and $B(M1)/B(E2)_{\textrm{in}}$]  in comparison with the experimental data are shown in Fig.~\ref{fig:reproduce}.
The four adopted parameter sets of the MOI in Table~\ref{tab:Pd105MOIset} and the corresponding results in Fig.~\ref{fig:reproduce} are denoted as (A), (B), (C), and (D), respectively.
For the energy spectra, the results of four sets of parameters are all in good agreement with the experimental data. The wobbling energies obtained by four parameter sets can reproduce the decreasing trend with spin from $I=13/2\hbar$ to $29/2\hbar$. The increasing trend of wobbling energies in the region $I \geq 33/2\hbar$ was attributed to three quasiparticle configuration in Ref.~\cite{Pd105}. Here the trends of wobbling energy at the whole spin region can also be described with one quasiparticle configuration adopted parameters (C) and (D).

The $\Delta I=1$ transitions connecting the wobbling bands should be dominated by an $E2$ component, due to the collective motion of the entire nuclear charge.
The strong $E$2 component of such transitions in $^{105}$Pd and the reduced transition probability ratios $B(E2)_{\textrm{out}}/B(E2)_{\textrm{in}}$ and $B(M1)/B(E2)_{\textrm{in}}$ are reproduced by the present calculation with the four sets of parameters. $B(E2)_{\textrm{out}}/B(E2)_{\textrm{in}}$ depends on $Q^{'}_{20}$ and $Q^{'}_{22}$ in Eq.~(\ref{Q0}), which is associated with $\gamma$ values.  It is found that $B(E2)_{\textrm{out}}/B(E2)_{\textrm{in}}$ will be significantly underestimated if a small $\gamma$ parameter is adopted in the calculation.

\subsection{Realization of transverse wobbling}

In the lowest row of  Fig.~\ref{fig:reproduce}, the expectation values of the core angular momentum components along the $m$, $s$, and $l$ axes are plotted. For parameter set (A), the value of ${\cal J}_m$ is close to ${\cal J}_s$, which agrees with the rigid-body model. For the yrast band, the core angular momentum increases along the $s$ axis more than that along the $m$ axis. For the yrare band, the $s$ and $m$ components of the core angular momentum are about the same. This is consistent with a tilt of core angular momenta about the $s$ axis.
For the parameter set (D), where the ratio ${\cal J}_m/{\cal J}_s=1:0.3$ is closed to that of hydrodynamical model, the component of the core angular momentum  is mainly on the $m$ axis for yrast and yrare bands. For the parameter sets (B) and (C), the angular momentum orientation with the minimal energy gradually transfers from the $s$ axis to the $m$ axis.

These different orientations of angular momentum are driven by the competition between the Coriolis term and rotational term to minimize energy.
As the valence nucleon angular momentum is mainly along the $s$ axis, the Coriolis term $-\hat{I}_{k}\hat{j}_{k}/{\cal J}_{k}$ contributes the most (least) to the energy  when the total angular momentum is along the $s$ ($m$) axis.
For the rotational term $\hat{I}_{k}^{2}/2{\cal J}_{k}$, it is largest (smallest) when the total angular momentum is along the $s$ ($m$) axis.
The MOI has a great influence on the orientation of core angular momentum.

To further illustrate the angular momentum geometry of
the wobbling motion, a probability profile on the $(\theta, \varphi)$
plane, $i.e.$, azimuthal plot~\cite{Streck18,CFQ17,CQB18,CQB19}, is provided in the following for both the angular momentum of nucleus and the valence nucleon.

In Figs.~\ref{fig:Aplota}-\ref{fig:Aplotd}, the obtained profiles $\mathcal{P}(\theta, \varphi)$ are shown at $I=11.5, 15.5$, and $19.5 \hbar$ for the yrast band and at $I=12.5,16.5$, and $20.5 \hbar$ for the yrare band with the four parameter sets of MOI in Table~\ref{tab:Pd105MOIset}. The distributions $\mathcal{P}(\theta, \varphi)$ of angular momentum are always concentrated around $\theta=90^{\circ}$.
This is because the angular momentum is prone to locate in the $sm$ plane to obtain the lowest energy.
To make it more visualized, the probability distribution of angular momenta in the $sm$ plane ($\theta=90^{\circ}$) are shown in the lower panels of Figs.~\ref{fig:Aplota}-\ref{fig:Aplotd}.
The radial coordinate represents the magnitude of angular momentum ranging from 0 to 21$\hbar$, and the angle coordinate $\varphi$ from $0^{\circ}$ to $360^{\circ}$.
The corresponding probabilities in the upper and lower panels have the same color schemes.

Adopted the different parameter sets of the MOI in Table~\ref{tab:Pd105MOIset}, distinct patterns of angular momentum are obtained in the calculations.
In Fig.~\ref{fig:Aplota}, the $\mathcal{P}(\theta, \varphi)$ results with parameter set (A) are shown, where the MOI is close to the rigid-body model. The maximum of $\mathcal{P}(\theta, \varphi)$ of the total and valence nucleon angular momentum are always located at $\varphi=90^{\circ}$, namely along the $s$ axis for $I=11.5\hbar, 15.5\hbar, 19.5\hbar$ in the yrast band.
For the yrare band, the total angular momentum has the maximal probabilities lying symmetrically with respect to the $s$ axis. While the angular momentum of valence nucleon still locates on the $s$ axis.
Combined with the orientation of the two,
it is straightforward to indicate the geometry of core angular momentum.
The core angular momentum aligns along the $s$ axis in the yrast band,
the motion in the yrare band corresponds to the oscillation (wobble) between two symmetrically orientations of angular
momentum about the $s$ axis.
Similar azimuthal plots  had been obtained in previous works, $e.g.$, Refs.~\cite{CQB19,Streck18,Ba130}, which were regarded as TW motion. They mentioned that the maximal probabilities of yrare states lying on a rim around the minimum reflects the wobbling motion (or precession) in this way~\cite{CQB19,Ba130}.  We denote such rotational mode as mode I in present work and visualize it in Fig.~1(d). Considering that it is to some extent different from the precession of the ideal TW picture, we discuss in detail the difference in Sec. IIIC.

With the increase of ratio ${\cal J}_m/{\cal J}_s$, the rotational mode I emerges at  $I=12.5\hbar$ and $I=16.5\hbar$ as shown in Fig.~\ref{fig:Aplotb}, and  $I=12.5\hbar$  in Fig.~\ref{fig:Aplotc}. For higher spins, rotational mode II shown in Fig.~\ref{fig:picture}(e) appears. It is a planar tilted rotation in the $sm$ plane for both yrast and yrare band, and
the tilted directions become closer to the $m$ axis compared with the excited states of mode I. This is reflected by the larger $\varphi$ values of the maxima of $\mathcal{P}(\theta, \varphi)$.
In Ref.~\cite{Pd105}, the parameters ${\cal J}_{m}:{\cal J}_{s}:{\cal J}_{l}=1:0.63:0.22$ with $b=0.023$ were adopted, which are close to sets (B) and (C). The mode I
could be obtained for spin region $I\leq 29/2\hbar$ if such parameters are adopted,  which coincides with the conclusion of TW motion in Ref.~\cite{Pd105}.

For set (D) where ${\cal J}_m$ is significantly larger than ${\cal J}_s$ and close to hydrodynamical MOI, the results are illustrated in Fig.~\ref{fig:Aplotd}.
The $\varphi$ coordinates of the maxima of $\mathcal{P}(\theta, \varphi)$ for total angular momentum approach $0^{\circ}$ and  $180^{\circ}$ at $15.5\hbar$ of the yrast band.
For the excited state $16.5\hbar$ of the yrare band, the total angular momentum oscillates slightly with respect to the $m$ axis. It is indicated the core angular momentum $\textit{\textbf{R}}$ arises a wobble about the $m$ axis which is achieved by adding angular momentum component along the $s$ axis. This mode is called mode III and shown in Fig.~\ref{fig:picture}(f).
With the increasing spin, the distributions of the valence nucleon angular momenta are more diffuse.
Since the Coriolis force tends to realign $\textit{\textbf{j}}$ to the orientation of $\textit{\textbf{I}}$, the $m$ axis is preferred by valence nucleon angular momentum instead of $s$ axis at $I=19.5\hbar$ of the yrast band.
As the valence nucleon go back to the $s$ axis at $I=20.5\hbar$, the yrare band still maintains mode III.
Mode III is different from the LW mode shown in Fig.~\ref{fig:picture}(c), where the valence nucleon angular momentum steadily aligns along the $m$ axis.

The corresponding relationship of the azimuthal plots in Figs.~\ref{fig:Aplota}-\ref{fig:Aplotd} and the geometry of angular momentum  shown in Fig.~\ref{fig:picture} is summarized in Table~\ref{tab:pictureset}.
Based on the above discussion of the results adopted four sets of parameters,
we get the case which can be approximately represented as the TW motion when the ratio ${\cal J}_m/{\cal J}_s$ is closer to that of rigid-body MOI. The LW motion is approximately appear when the ratio is close to that of hydrodynamical MOI.
The variation of these angular momentum geometries is dependent on the values of  MOI, especially the ratio ${\cal J}_m/{\cal J}_s$. The mechanism of rotational bands in $^{105}$Pd might be associated with one of these modes or a mixture.
The present results also suggest that the
available data may not be sufficient to identify the TW mechanism, and further experimental explorations such as lifetime or
$g$-factor measurements are expected.

In Table~\ref{table:MOI}, we summarize the adopted MOI in the study of wobbling band based on PRM in the previous works, and the corresponding suggested wobbling modes. It can be seen that the calculations for $^{161,163,165,167}$Lu~\cite{Raduta2020PRC} and $^{187}$Au~\cite{Au187}, in which the adopted ${\cal J}_m/{\cal J}_s$ close to hydrodynamical MOI, have suggested the LW mode.
If the ratio is close to the rigid MOI or between the hydrodynamical and rigid MOI, then TW mode is in general suggested by PRM for $^{105}$Pd~\cite{Pd105}, $^{130}$Ba~\cite{Ba130}, $^{135}$Pr~\cite{Pr135,Frauendorf14,La133}, $^{163}$Lu~\cite{Frauendorf14}, and $^{183}$Au~\cite{Au183}.
Our conclusion from the study of $^{105}$Pd is not in conflict with the the previous calculated results and gives the relationship of  MOI and wobbling modes. However, the character of the nuclear MOI is a longstanding problem in the research of rotational band. Recently, both of the empirical MOI extracted experimentally~\cite{Allmond17} and the theoretical MOI calculated by the microscopic cranking model~\cite{Frauendorf182} suggested that the ratios of MOI follow the hydrodynamical model. If the hydrodynamical MOI is adopted, the TW mode seems to be difficult to occur from the above discussion.
The further understanding of MOI is a key point to clarify the debates on TW mode.

\subsection{Precession or tunneling}

Precession of the nucleus means that  the  orientation of the total angular momentum is rotating about a principal axis.
Such precession has always been considered in the discussions about the TW, LW, or the tilted precession, as shown in Figs.~\ref{fig:picture}(a), \ref{fig:picture}(b), and \ref{fig:picture}(c). It should be noted the classical trajectories of  angular momentum for precession might change to tunneling in the quantum system.

To address
this issue, we provide the classical trajectories and the quantum probability density distribution of angular momentum in Fig.~\ref{fig:trajectory}. Here, we plot the case of purely collective rotor to avoid the ambiguity due to coupling of a particle to a rotor core.
The classical orbits of angular momentum are obtained from  the intersection of the angular momentum sphere
$R_{m}^{2}+R_{s}^{2}+R_{l}^{2}=R(R+1)$
with the energy ellipsoid
$R_{m}^{2}/{\cal J}_{m}+R_{s}^{2}/{\cal J}_{s}+R_{l}^{2}/{\cal J}_{l}=2E$~\cite{Landau,Lawrie20,Frauendorf14}.
For the quantum probability density distribution of angular momentum, it is obtained by the quantum triaxial rotor model~\cite{Bohr75} with  the probability distribution calculated by Eq.~(\ref{APlot}).
In Figs.~\ref{fig:trajectory}(a), \ref{fig:trajectory}(b), \ref{fig:trajectory}(c) and \ref{fig:trajectory}(d), the ratios of MOI ${\cal J}_{m}/{\cal J}_{s}/{\cal J}_{l}$ are adopted respectively as $1/0.25/0.25$, $1/0.33/0.18$, $1/0.43/0.12$, and $1/0.54/0.07$. These ratios are corresponding to the hydrodynamical MOI with $\gamma=30^{\circ},25^{\circ},20^{\circ},15^{\circ}$.
The obtained energy $E$ calculated by quantum triaxial rotor model for spin $13\hbar$ are respectively $1.48, 1.48, 1.49$, and $1.51$ MeV, which are input to get the classical trajectories.

The classical trajectories  and quantum probability density distribution  of the angular momentum are circles only in the case of ${\cal J}_{s}={\cal J}_{l}$, as shown in Fig.~\ref{fig:trajectory}(a).
In general, the classical trajectory are not circles, as shown in Figs.~\ref{fig:trajectory}(b), \ref{fig:trajectory}(c), and \ref{fig:trajectory}(d). Correspondingly,
the maximum probabilities of the angular momentum locate at two symmetrically points about the $m$ axis in the quantum case. A tunneling should occur if the barrier between them is high enough.
Thus,  precession and tunneling are two aspects of the quantum wobbling motion.
Modes I, II, and III in our calculation for $^{105}$Pd, as shown in Figs.~\ref{fig:picture}(d), \ref{fig:picture}(e), \ref{fig:picture}(f), exhibit a tunneling between two symmetrically
orientations of angular momentum for the yrare band.
It seems that the tunneling between two orientations of angular momentum is preferable to constitute the TW and LW.

\section{Summary}

We have reinvestigated the reported  TW band in an odd-mass nucleus $^{105}$Pd based on the triaxial particle rotor model.
The experimental data of wobbling band could be
reproduced by the calculated results adopting different parameter sets of MOI. By analyzing the azimuthal plot of the angular momentum of nucleus and valence nucleon, different types of rotational modes are shown.
It is confirmed that these modes are sensitive to the ratio between the MOI at the $m$ and $s$ axis, namely  ${\cal J}_{m}/{\cal J}_{s}$.
The TW mode appears approximately when the ratio agrees with the rigid-body MOI, $i.e.$, the total angular momentum   wobbles around the $s$ axis.
When the ratio agrees with the hydrodynamical MOI, a wobbler around the $m$ axis occurs. When the ratio is between the above two, the planar tilted rotation occurs for both of the yrast and yrare band.
The mechanism of rotational bands in $^{105}$Pd might be one of these three modes. In addition, it is exhibited that
precession and tunneling are two aspects of the quantum wobbling motion. The tunneling aspect dominates
in the present yrare states of $^{105}$Pd.
The further understanding of nuclear MOI in theory is necessary to clarify the debates on wobbling motion, and further experimental explorations to identify the TW mechanism are also expected.

\begin{acknowledgments}
This work is partly supported by the Major Program of Natural Science Foundation of
Shandong Province (No.~ZR2020ZD30), the Outstanding Youth Fund of Natural Science Foundation
of Shandong Province (ZR2020YQ07), the National Natural Science Foundation of China
(No.~11675094, No.~12075137, No. 12075138), and the Shandong Natural Science Foundation (No.~ZR2020QA084).
\end{acknowledgments}

\clearpage

redpajama_set_name: RedPajamaArXiv


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